AMCS, A Glazov, V Radescu, S Whitehead, A Sapronov

Slides:



Advertisements
Similar presentations
Low-x and PDF studies at LHC Sept 2008 A M Cooper-Sarkar, Oxford At the LHC high precision (SM and BSM) cross section predictions require precision Parton.
Advertisements

May 2005CTEQ Summer School1 Global Analysis of QCD and Parton Distribution Functions Dan Stump Department of Physics and Astronomy Michigan State University.
Precision Measurement of F 2 with H1 Workshop on DIS and QCD, Florence, Max Klein for the H1 Collaboration Towards today The Measurement Results.
HERAPDF0.2 and predictions for W/Z production at LHC PDF4LHC A M Cooper-Sarkar 29 May 2009 Motivation Some of the debates about the best way of estimating.
Road to CTEQ7 J. Huston CTEQ meeting. Roadmap CTEQ6 was published in 2002, followed by CTEQ6.1 in 2003 Pavel has given you a review of CTEQ6.6 which will.
H1/ZEUS fitters meeting Jan 15 th 2010 Am Cooper-Sarkar Mostly about fitting the combined F2c data New work on an FFN fit PLUS Comparing HERAPDF to Tevatron.
HERAPDF0.2 and predictions for W/Z production at LHC PDF4LHC A M Cooper-Sarkar 29 May 2009 Motivation Some of the debates about the best way of estimating.
QCD Studies in ATLAS Martin Siebel (CERN) On behalf of the ATLAS Collaboration XIII Lomonosov Conference, Moscow,
Preliminary results in collaboration with Pavel Nadolsky Les Houches /6/5.
Why are PDF’s important for ATLAS Durham, Sep 18 th 2006 A M Cooper-Sarkar, Oxford SM CSC notes UK effort Min bias Glasgow, Sheffield W/Z cross-section.
PDF’s for the LHC: LHC cross section benchmarking and error prescriptions J. Huston Michigan State University MCTP Spring Symposium on Higgs Boson Physics.
Update on fits for 25/3/08 AM Cooper-Sarkar Central fit: choice of parametrization Central fit: choice of error treatment Quality of fit to data PDFs plus.
Studying emission mechanisms of AGN Dr. Karsten Berger Fermi School, June ©NASA.
The New HERAPDF Nov HERA SFgroup AM Cooper-Sarkar Appears compatible with HERAPDF0.1 when doing fits at Q20=4.0 GeV2 But humpy gluon is Chisq favoured.
A few slides to summarise what Alessandro and I were up to for March 24th video meeting Taking for granted that W+/- are good measurements to make- are.
May 14 th 2008 averaging meeting A M Cooper-Sarkar Look at the HERA-I PDFs in new ways Flavour break-up High-x Compare to ZEUS data alone/ H1 data alone.
PDF fitting to ATLAS jet data- a first look A M Cooper-Sarkar, C Doglioni, E Feng, S Glazov, V Radescu, A Sapronov, P Starovoitov, S Whitehead ATLAS jet.
Ronan McNulty EWWG A general methodology for updating PDF sets with LHC data Francesco de Lorenzi*, Ronan McNulty (University College Dublin)
Moving on to BSM physics Example of how PDF uncertainties matter for BSM physics– Tevatron jet data were originally taken as evidence for new physics--
Discussion of calculation of LHC cross sections and PDF/  s uncertainties J. Huston Michigan State University 1.
Further investigations on the fits to new data Jan 12 th 2009 A M Cooper-Sarkar Considering ONLY fits with Q 2 0 =1.9 or 2.0 –mostly comparing RTVFN to.
Treatment of correlated systematic errors PDF4LHC August 2009 A M Cooper-Sarkar Systematic differences combining ZEUS and H1 data  In a QCD fit  In a.
11 QCD analysis with determination of α S (M Z ) based on HERA inclusive and jet data: HERAPDF1.6 A M Cooper-Sarkar Low-x meeting June 3 rd 2011 What inclusive.
By Henry Brown Henry Brown, LHCb, IOP 10/04/13 1.
In the QCD sector the PDFs limit our knowledge - transport PDFs to hadron-hadron cross-sections using QCD factorization theorem for short-distance inclusive.
Future of DIS: PDF studies at LHC April 18 th DIS 2007 A M Cooper-Sarkar, Oxford At the LHC high precision (SM and BSM) cross section predictions require.
April 7, 2008 DIS UCL1 Tevatron results Heidi Schellman for the D0 and CDF Collaborations.
H1 and ZEUS Combined PDF Fit DIS08 A M Cooper Sarkar on behalf of ZEUS and H1 HERA Structure Function Working Group NLO DGLAP PDF fit to the combined HERA.
D Parton Distribution Functions, Part 2. D CT10-NNLO Parton Distribution Functions.
MSTW update James Stirling (with Alan Martin, Robert Thorne, Graeme Watt)
F Don Lincoln f La Thuile 2002 Don Lincoln Fermilab Tevatron Run I QCD Results Don Lincoln f.
Physics at the LHC M. Guchait DHEP Annual Meeting 7-8 th April, 2016.
1 Proton Structure Functions and HERA QCD Fit HERA+Experiments F 2 Charged Current+xF 3 HERA QCD Fit for the H1 and ZEUS Collaborations Andrew Mehta (Liverpool.
1 A M Cooper-Sarkar University of Oxford ICHEP 2014, Valencia.
Joshua Moss (Ohio State University) on behalf of the ATLAS Collaboration ICHEP 2012, Melbourne 6 July 2012 ATLAS Electroweak measurements of W and Z properties.
Developments in PDF4LHC Developments in PDF4LHC Albert De Roeck CERN, Geneva, Switzerland Antwerp University Belgium UC-Davis California USA BUE, Cairo,
Parton Distributions and Higgs Production at the LHC and the Tevatron James Stirling Cambridge University introduction: overview and recent developments.
HERAPDF1.0 and predictions for W/Z production at LHC PDF4LHC A M Cooper-Sarkar August 2009 Motivation Some of the debates about the best way of estimating.
1 Proton Structure and Hard QCD AM Cooper-Sarkar, Oxford Phys Rev D93(2016)
Klaus Rabbertz CPPM, Marseille, HERAFitter Meeting 1 The fastNLO Collaboration: Daniel Britzger, Thomas Kluge, Klaus Rabbertz, Fred Stober,Markus.
AM Cooper-Sarkar PDF4LHC July 4th 2010 HERAPDF fits update We have more combined H1 + ZEUS data: The low energy run data which was used to measure FL has.
28/04/2000 DIS Liverpool, April 28th 1 QCD with W/Z-events Ursula Bassler, LPNHE-Paris in behalf of the CDF and DØ collaborations Basics on W/Z.
Impacts and constraints on PDFs at ATLAS April 17th DIS 2007 A M Cooper-Sarkar, Oxford At the LHC high precision (SM and BSM) cross section predictions.
PDF studies at ATLAS HERA-LHC workshop 2007 A M Cooper-Sarkar, Oxford
PDFs from HERA to the LHC March 2005 A.M Cooper-Sarkar
Electroweak Physics Lecture 6
PDF uncertainties and LHC physics -using ATLAS examples A M Cooper-Sarkar Cambridge- 3rd June 2009 STANDARD MODEL There are W/Z ‘calibration’ measurememts:
Early EWK/top measurements at the LHC
J. Huston Michigan State University for CTEQ-TEA PDF fitting group
From the Tevatron to the LHC: Parton Distribution Functions (pdfs)
Michigan State University
Photon Cross Sections at Ecm=2TeV
News from HERAPDF A M Cooper-Sarkar PDF4LHC CERN March
New processes? New ideas
Another World Record Madrid, : 21.5 m of diameter, Paella for people!
HERA I - Preliminary H1 and ZEUS QCD Fit
HESSIAN vs OFFSET method
W Charge Asymmetry at CDF
PDF studies at ATLAS HERA-LHC workshop 2007 A M Cooper-Sarkar, Oxford
Low-x physics at the LHC
the CT10-NNLO Global Analysis
PDF4LHC: LHC needs February 2008 A M Cooper-Sarkar, Oxford
What we’ll discuss.. Techniques used to scale and compare from pp to NN Description of ingredients recipes used by experiments caveats and uncertainties.
May 14th 2008 averaging meeting A M Cooper-Sarkar
ATLAS 2.76 TeV inclusive jet measurement and its PDF impact A M Cooper-Sarkar PDF4LHC Durham Sep 26th 2012 In 2011, 0.20 pb-1 of data were taken at √s.
Dilepton Mass. Progress report.
Parton Density Functions
Ronan McNulty University College Dublin
A M Cooper-Sarkar and K Wichmann
Rick Field – Florida/CDF/CMS
Presentation transcript:

AMCS, A Glazov, V Radescu, S Whitehead, A Sapronov Confronting HERAPDF with Tevatron data and LHC data PDF4LHC march 7th 2011 A M Cooper-Sarkar +Tevatron W-asymmetry and Z0 rapidity spectrum +Tevatron jets--- with apologies to D0, so far only CDF data fitted LHCb lepton asymmetry CMS lepton asymmetry ATLAS lepton asymmetry AMCS, A Glazov, V Radescu, S Whitehead, A Sapronov

How good or bad is the HERAPDF description of the Tevatron data?. We usually just show you plots. Let’s calculate χ2- and then FIT the data. Can the error bands of HERAPDF!.5 cover the variation due to input of new data? The description of the CDF Z0 rapidity LOOKS OK but what is the χ2 for these data points to HERAPDF1.5 central values? 36/28 -acceptable But this does NOT account for the error band of the HERAPDF fit

So FIT the CDF Z0 rapidity data: χ2/ndp =30.5/28 And look to see if the resulting PDF has shifted outside error bands. Here the HERADF+CDF Z0 rapidity fit is the blue line– it does NOT move outside the HERAPDF1.5 error bands The fit is done with HERAPDF standard parametrisation BUT with the low-x Bdv parameter of the d-valence freed so that Bdv ≠ Buv (note this was one of our standard parametrisation variations)

The description of the CDF W-asymmetry LOOKS OK but what is the χ2 for these data points to HERAPDF 1.5 central values? 40/13 --not very good But this does NOT account for the error band of the fit

So FIT the CDF W-asymmetry data: χ2 = 21/13 And look to see if the resulting PDF has shifted outside our error bands. Here the HERADF+CDF W- asymmetry fit is the blue line– it does NOT move outside the HERAPDF1.5 error bands Note the χ2 is comparable to that of NNPDF 24/13 The fit is done with HERAPDF standard parametrisation BUT with the low-x Bdv parameter of the d-valence freed so that Bdv ≠ Buv Since the W-asymmetry measures uv-dv is is desirable to allow more freedom in the valence sector (note this was one of our standard parametrisation variations)

Sticking with W and Z data move to the LHC HERAPDF1.0 and 1.5 compared to LHCb lepton asymmetry data- no time to fit yet From G. Watt

HERAPDF1.5 compared to CMS lepton asymmetry data- go the data points from La Thuile no time to fit yet- but it looks pretty good Pt lepton > 25 GeV? Also Etmiss > 25 GeV?

HERAPDF1.5 compared to ATLAS muon asymmetry data– this I have had time to fit(!) What is the χ2 for these data points to HERAPDF 1.5 central values? 27/11 --not very good But this does NOT account for the error band of the fit Ptmuon > 20 GeV Et miss > 25 GeV

So FIT the ATLAS muon asymmetry data: χ2 = 13.5/11 And look to see if the resulting PDF has shifted outside our error bands. Here the HERADF+CDF W- asymmetry fit is the blue line– it does NOT move outside the HERAPDF1.5 error bands The fit is done with HERAPDF standard parametrisation BUT with the low-x Bdv parameter of the d-valence freed so that Bdv ≠ Buv Since the W-asymmetry measures uv-dv is is desirable to allow more freedom in the valence sector (note this was one of our standard parametrisation variations)

Now return to Tevatron jets The description of the D0 jet data LOOKS OK but what is the χ2 for such jet data to HERAPDF1.5 central values?

Table from G Watt The χ2 to these CDF data for HERAPDF1.5 is 176/76 –close to Watt’s value for HERAPDF1.0 – not surprising since high-x gluon does not change much 1.0 to 1.5

After fitting these CDF jet data the χ2= 113/76 And look to see if the resulting PDF has shifted outside our error bands. Here the HERADF+CDF D0 rapidity fit is the blue line– it does NOT move much outside the HERAPDF1.5 error bands- does have a hard high-x gluon- at the edge of the error band. Better χ2 would come from the use of the flexible parametrisation and free alphas… future work

But of course we are working on improved HERAPDF fits The message is that the HERAPDF1.5 describes the Tevatron and early LHC data well – within its error bands But of course we are working on improved HERAPDF fits And NNLO HERAPDF1.5f with uncertainty bands is on its way..

extras

Fit to CDF jets data with very flexible paraemtrisation Chisq= 78/76.. But outside HERAPDf1.5 ! Could also try fitting alphas on less flexible param